Tire and wheel noise reducing device and system

ABSTRACT

A system for dissipating sound shock waves within a vehicle tire includes a wheel upon which a tire is mounted to create an internal air chamber defined by the wheel and the tire. A flow-resistant barrier is coupled to the wheel or the tire and defines an air cavity within the internal air chamber. The barrier comprises a material that provides an acoustical resistance to sound shock waves passing therethrough. The air cavity defined by the barrier has a volume such that air within the cavity offers relatively small impedance to the passage of shock waves through the barrier and into the air cavity. The barrier also can produce frictional heat when displaced by a shock wave, thereby converting energy of the shock wave to heat to reduce noise associated therewith.

RELATED APPLICATION

This patent application claims priority under 35 U.S.C. § 119 to U.S.Provisional Patent Application No. 60/694,018 entitled “Tire and WheelNoise Absorbing Device and System,” filed Jun. 24, 2005. The completedisclosure of the above identified priority application is hereby fullyincorporated herein by reference.

TECHNICAL FIELD

The present invention relates generally to reducing vehicle noise fromtires and wheels. Specifically, the present invention relates to asound-reducing device disposed in the internal air chamber created by atire and a wheel upon which the tire is mounted.

BACKGROUND OF THE INVENTION

When car tires contact a road surface, they generate considerable noise.At speeds above 25 mph in certain vehicles, tire noise can be greaterthan all other sources of automotive noise combined. Accordingly, carand tire manufacturers spend large amounts of resources every year onresearch and development to reduce tire noise.

Tire noise results from many sources. For example, tire noise resultsfrom (1) low-frequency shock waves produced by excitation of theinternal tire air chamber from tire deformation caused by the contact ofthe tire with the road surface; (2) low-frequency tire structure ringingdue to air chamber excitation caused by the deflection of the tire atroad contact; (3) high-frequency external tread air compression causedby air temporarily trapped between the tread and the road surface; and(4) high-frequency contact scrub caused by the friction between the tireand the road surface.

Some tread air compression noise is not avoidable. For example, treadair compression acts to clear water from the tread contact surface bycompressing the water and air at road contact and then expanding themixture at tread release. Additionally, some contact scrub noise is notavoidable because tires have finite adhesion which generates frictionand noise with the road surface.

Shock wave energy from tire deformation is transmitted from the treadcontact area into the internal tire air chamber created by the tire andthe wheel upon which the tire is mounted. The energy transmitted intothe internal tire air chamber is only dissipated by tire ringing andcoupling of the noise to the wheel. Such tire ringing and noise couplingcomprise a large portion of the total amount of tire noise.

Conventional methods for reducing tire noise have several deficiencies.In particular, those methods do not effectively absorb low-frequencyenergy (e.g., below 800 Hz) associated with the shock waves that producetire noise. As tires generate significant low-frequency energy, anefficient tire noise absorber should reduce the noise produced by suchlow-frequency energy. However, conventional methods do not adequatelyreduce that noise. Additionally, low-frequency noise increases perceivedhigh frequency noise produced by tread air compression and tire scrub.Accordingly, conventional methods fail to reduce the perceived highfrequency tire noise by failing to reduce low-frequency energy noise.Other deficiencies include the difficulty of mounting a tire to a wheelwhen using a conventional method, the possible damage if theconventional method fails during vehicle operation, and the inefficiencyof conventional methods.

Conventional low-frequency noise absorbing methods exist. However, suchconventional methods are not practical for small internal air chambers,such as a tire's air chamber. Such conventional low-frequency absorbingmethods are too large for a tire air chamber, would prevent tireinflation, are not efficient, and/or pose safety hazards if used incombination with a tire.

Accordingly, a need exists in the art for reducing noise generated by orwithin tires and the wheels upon which the tires are mounted.Particularly, a need exists in the art for reducing tire noise byabsorbing or reducing energy in the internal air chamber of a tire. Moreparticularly, a need exists for a tire noise absorber/reducer that canabsorb or reduce low frequency energy while operating inside a smallinternal air chamber, such as a tire's air chamber.

SUMMARY OF THE INVENTION

A device for reducing tire noise can absorb and reduce low-frequencyenergy that produces tire noise. The device can absorb sound shock wavesby alternately pressurizing and depressurizing a vessel having an airflow-resistant barrier. The flow-resistant barrier dampens pressureflows into and out of the vessel to dampen shock waves that pass throughthe barrier. Additionally, friction in the flow-resistant element of thevessel converts sound energy into heat, thus attenuating the sound.Additionally, a hybrid device can have elements of an air flow-resistantcavity absorber and elements of a frictional absorber.

According to one aspect, a tire noise absorbing device can comprisemultiple layers of an air flow-resistant material with multiple openingsin each layer. The layers can be assembled such that the openings ofeach layer are offset with respect to overlapped portions of an adjacentlayer. The offset openings allow air to pass through the layers when thetire is stationary and the layers are slack, thereby allowing completeinflation of the tire. The overlapping layers can be coupled to a wheelor directly to a tire to form loops of overlapped elements. When a caris put into motion and the tire begins to rotate, centrifugal forceforces the overlapped layers outward and together to seal the airpassages of the openings and to form an air flow-resistant cavitybetween the wheel and the cloth layers. Specifically, the inner layer isforced outward against the outer layer, the openings in the inner layerare sealed by the outer layer, and the openings in the outer layer aresealed by the inner layer. The layers restrict air flow between a tire(outer) side of the layers and a wheel (inner) side of the layers,thereby absorbing low-frequency energy noise as air passes through thelayers.

In a further embodiment, the layers can slide against each other andcreate friction when displaced by low-frequency shock waves. Theresulting friction can absorb additional low-frequency energy noise bydissipating such the shock waves via heat produced by the friction.

Increasing the absorption of low-frequency energy also can reduce theperceived high-frequency tire noise without compromising tread design ortire adhesion. The design can fit easily into an existing tire and canbe mounted to existing wheels or to a tire during or after themanufacturing process.

Other aspects include variations of the position and coupling means ofattaching the device to the wheel or tire. For example, the device canbe coupled at a centrally located position on the wheel or with variousprofiles that provide different shaped flow-resistant cavities. Stillother aspects include multiple elements with overlapping or interlockingends to create the flow-resistant cavity. These elements are forcedoutward by centrifugal force and create a cavity when the overlapping orinterlocking portions move together to create a device that resists airflow. In addition, the overlapping portions can create friction whendisplaced by shock waves to further absorb low frequency noise. Yetanother aspect includes creating multiple flow-resistant air cavities bylayering two or more flow-resistant elements around a wheel or tire.These multiple flow-resistant air cavities can absorb shock waves andcan improve noise reduction. Further aspects involve a tubular,crescent, or curved element positioned on the wheel or tire, thuscreating a single flow-resistant cavity. Such an element in the tubularshape also can be used in sections to create multiple flow-resistantcavities around the wheel.

The described devices can be coupled to the wheel or tire in a varietyof ways. For example, the elements that create the flow-resistant cavitycan be coupled to the wheel or tire with adhesive or clamps, by beingcrimped into a groove or flange in the wheel or tire, or by beingwelded, molded, or weaved into the wheel or tire.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A is a perspective view illustrating a tire noise absorbing systemcomprising a flow-resistant barrier disposed on a wheel for a tireaccording to an exemplary embodiment.

FIG. 1B is a cross-sectional view of the exemplary system illustrated inFIG. 1A.

FIG. 2 illustrates features of the layers of the tire noise absorbingsystem illustrated in FIGS. 1A and 1B according to an exemplaryembodiment.

FIG. 3A is a perspective view illustrating a tire noise absorbing systemcomprising a flow-resistant barrier disposed on a wheel for a tireaccording to another exemplary embodiment.

FIG. 3B a cross-sectional view of the exemplary system illustrated inFIG. 3A.

FIG. 4A is a perspective view illustrating a tire noise absorbing systemcomprising a flow-resistant barrier disposed on a wheel for a tireaccording to yet another exemplary embodiment.

FIG. 4B is a cross-sectional view of the exemplary system illustrated inFIG. 4A.

FIG. 5 is a perspective view illustrating a tire noise absorbing systemcomprising multiple elements that create a flow-resistant barrieraccording to an exemplary embodiment.

FIG. 6A a perspective view illustrating a portion of a tire noiseabsorbing system comprising multiple elements that create aflow-resistant barrier according to another exemplary embodiment.

FIG. 6B is a side view of the exemplary system illustrated in FIG. 6A.

FIG. 7 is a perspective view illustrating a tire noise absorbing systemcomprising discontinuous elements coupled to a wheel according to anexemplary embodiment.

FIG. 8A is a perspective view of a tire noise absorbing systemcomprising multiple elements that create a flow-resistant barrieraccording to an exemplary embodiment.

FIG. 8B is a cross-sectional view of the exemplary system illustrated inFIG-8A.

FIG. 9A is a perspective view illustrating a tire noise absorbing systemcomprising two or more elements that create multiple flow-resistantbarriers according to an exemplary embodiment.

FIG. 9B is a cross-sectional view of the exemplary system illustrated inFIG. 9A.

FIG. 10 is a perspective view illustrating a tire noise absorbing systemcomprising a tubular air flow-resistant barrier according to anotherexemplary embodiment.

FIG. 11 is a perspective view illustrating a tire noise absorbing systemcomprising a continuous flow-resistant barrier according to an exemplaryembodiment.

FIG. 12 is a perspective view illustrating a tire noise absorbing systemcomprising multiple tubular air flow-resistant barriers according to anexemplary embodiment.

FIG. 13 is a perspective view illustrating a representative element thatcan be used in any embodiment illustrated in FIGS. 1-12 and 14 accordingto an exemplary embodiment.

FIG. 14 is a cross-sectional view of a tire noise absorbing systemcomprising a flow-resistant barrier coupled to a tire mounted to a wheelaccording to an exemplary embodiment.

DETAILED DESCRIPTION OF EXEMPLARY EMBODIMENTS

Exemplary embodiments will be described with reference to FIGS. 1-13 inwhich the same reference numerals represent similar elements.

FIG. 1A is a perspective view illustrating a tire noise absorbing system100 comprising a flow-resistant barrier disposed on a wheel 140 for atire 160 according to an exemplary embodiment. FIG. 1B is across-sectional view of the exemplary system 100 illustrated in FIG. 1A.As shown in FIGS. 1A and 1B, the system 100 comprises multiple,overlapped layers 110, 120 of material, which form an acousticflow-resistant barrier. The layer 110 comprises an outer layer withreference to the wheel 140, and the layer 120 comprises an inner layerwith reference to the wheel 140. The overlapping layers 110, 120 arecoupled to the wheel 140 along their edges at location 150 to form loopsof overlapped material. In other words, the layers 110, 120 are wrappedaround the wheel 140 and coupled to both sides of the wheel 140 atlocations 150. The location 150 indicates any suitable location on thewheel 140 for coupling the flow-resistant barrier thereto.Alternatively, the layers 110, 120 can be coupled directly to a tire 160in a similar fashion such that they form loops of overlapped absorptiveelements for a flow-resistant barrier (see FIG. 14 discussedhereinafter).

In the exemplary embodiment illustrated in FIGS. 1A and 1B, both edgesof the layers 110, 120 are attached to opposite sides of the wheel 140with enough slack to allow centrifugal force to force the layers 110,120 outward to create the flow-resistant barrier defined by the layers110, 120. The flow-resistant barrier defines an inner air cavity 170 inan internal tire air chamber defined by the tire 160 and the wheel 140.Thus, the flow-resistant barrier divides the internal tire air chamberinto an inner air cavity 170 and an outer air cavity 180. The barrierdefined by the layers 110, 120 is flow-resistant because the layers 110,120 resist air flow between the outer air cavity 180 and the inner aircavity 170. In an exemplary embodiment, the volume of the inner aircavity can have a volume that is in a range of about 8% to about 40% ofthe total internal tire air chamber volume. Other cavity volumes aresuitable. The volume of the inner air cavity 170 can be sized so thatthe air therein provides little resistance to the flow of sound shockwaves from the outer air cavity 180 through the layers 110, 120 to theinner air cavity 170.

Thus, the barrier comprises a material that provides an acousticalresistance to sound shock waves passing therethrough. The inner aircavity 170 defined by the barrier has a volume such that air within theinner air cavity 170 offers relatively small impedance to the passage ofshock waves through the barrier and into the inner air cavity 170. Inoperation, sound shock waves are produced in the outer air cavity 170 asthe tire travels over a road. The sound shock waves travel toward theinner air cavity 170 and encounter the flow-resistant barrier defined bythe layers 110, 120. As the sound shock waves pass through the barrier,the barrier absorbs energy from those shock waves due to the acousticalimpedance of the barrier. Initially, the air within the inner air cavity170 offers relatively small impedance to the passage of shock wavesthrough the barrier and into the inner air cavity 170. As shock wavescontinue to pass through the barrier and into the inner air cavity 170,the inner air cavity 170 becomes pressurized with respect to the outerair cavity. At this point, the air in the inner air cavity 170 canimpede the passage of shock waves through the barrier and into the innerair cavity 170. When the inner air cavity pressure becomes greater thanthe outer air cavity pressure, the inner air cavity 170 willdepressurize as air flows out of the inner air cavity 170 to the outerair cavity 180. That process continues while the tire is in motion.Additionally, sound shock waves that pass through the flow-resistantbarrier and are reflected by the wheel 140 will pass back through theflow-resistant barrier to the outer air cavity 180. The flow-resistantbarrier will absorb further energy from the sound shock waves duringthat process, further reducing noise associated therewith. The barrieralso can reduce noise associated with the sound shock waves byconverting energy from those shock waves into frictional heat, asdiscussed in more detail hereinafter.

The layers 110, 120 restrict but not prevent air flow between the outerair cavity 180 and the inner air cavity 170. Accordingly, the layers110, 120 provide acoustical impedance by resisting the flow of soundshock waves therethrough. In exemplary embodiments, the layers 110, 120,can comprise flexible cloth. For example, the layers 110, 120 cancomprise Kevlar, cotton, Spectra, silk, fiberglass, or any othersuitable material. Such suitable materials generally include a weave orstructure that restricts air flow through the material based on thespace tightness of the weave or structure of the material.

In an exemplary embodiment, the layers 110, 120 can comprise a materialhaving a weave with a porosity ranging from about 10% to about 50%cavity fill at cavity saturation, based on the resonant energy in aclosed tire cavity. “Cavity fill at cavity saturation” describes thelength of time required to pressurize the inner air cavity 170 by soundshock waves passing through the flow-resistant barrier formed by thelayers 110, 120. The time it takes to fill or empty the inner air cavity170 determines the limit of low frequency absorption of the system 100.Other porosities are suitable. For example, an alternative suitableporosity to pressurize the inner air cavity 170 is from about 10% toabout 75% at low frequencies. The lower frequency performance of aflow-resistant absorber depends on the size of the inner air cavity 170and the efficiency of the resistance of the flow-resistant barriercreated by the layers 110, 120. Flow resistance depends on the porosityof the material of the layers 110, 120. As the cavity fills with airfrom the sound shock waves passing through the flow-resistant barrier,the pressure resistant cavity absorber can reach a lower frequency limitbased. The low frequency limit is established based on the time it takesfor the inner air cavity 170 to fill or empty. The larger the inner aircavity 170, the lower the frequency limit. In an exemplary embodiment,the acoustical resistance of the flow-resistant barrier and the size ofthe inner air cavity 170 will allow acoustical sound waves to passthrough the barrier quickly enough to reduce the noise associatedtherewith, but slowly enough to allow the inner air cavity 170 to becomefully pressurized. The inner air cavity 170 is fully pressurized when ithas reached the same pressure as the pressure caused by the acousticalsound waves. As the energy absorber of the system 100 is disposed withina pressurized air chamber (i.e., the internal tire air chamber), thesystem 100 can comprise a smaller air cavity than would be needed atnormal atmospheric pressure.

In the exemplary embodiment illustrated in FIGS. 1A and 1B, theapertures 130 comprise slits formed in the layers 110, 120. Theapertures 130 in each layer 110, 120 are offset such that the openingsin adjacent layers 110, 120 do not overlap. When the wheel 140 isstationary, the layers 110, 120 are slack. In that state, the apertures130 allow air to pass therethrough, thereby allowing complete inflationof the internal tire air chamber. Complete inflation means inflation ofthe outer air cavity 180 between the tire and the layers 110, 120 andthe inner air cavity 170 between the layers 110, 120 and the wheel 140.The apertures 130 can comprise any suitable geometry that allows thelayers 110, 120 to conform to the wheel 140 and that allows air to passbetween the layers 110, 120 for tire inflation.

In an exemplary embodiment, the layers 110, 120 can be coupled directlyto the wheel 140 at location 150 using an adhesive. For example, theadhesive can comprise epoxy or other any other suitable adhesive forattaching the layers 110, 120 to the wheel 140. The adhesive can beselected based on the particular application to adhere the layers 110,120 to the wheel 140 and to resist the centrifugal force generated bythe rotation of the wheel 140 and heat generated within the internaltire air chamber.

In alternative exemplary embodiments, other suitable methods can be usedto couple the layers 110, 120 to the wheel 140. For example, the layers110, 120 can be crimped into a groove (not shown) or flange (not shown)attached to or molded in the wheel 140. Alternatively, the layers 110,120 can comprise a metal flange (not shown) along the edge of the layers110, 120, and the flange can be welded around or otherwise coupled tothe wheel 140.

As depicted in FIGS. 1A and 1B, the system 100 can comprise two layers110, 120. However, additional layers can be used in alternativeexemplary embodiments. For example, the system 100 can comprise three ormore layers. The layers can be assembled such that the apertures 130between adjacent layers are offset and do not overlap.

FIG. 2 illustrates features of the layers 110, 120 of the tire noiseabsorbing system 100 illustrated in FIGS. 1A and 1B according to anexemplary embodiment. As shown, the layers 110, 120 of the system 100comprise continuous layers of flat material with multiple apertures 130in each layer. In an exemplary embodiment, the openings can be spaced ina range of about 1 to about 5 inches apart. Other spacing between theopenings is suitable. The continuous layers can be wrapped around andattached to the wheel 140 as illustrated in FIGS. 1A and 1B.

In an alternative exemplary embodiment (not illustrated in FIGS. 1A, 1B,2, and 14), each layer 110, 120 can comprise multiple strips of materialdisposed adjacent to each other and overlapped to form the apertures130. In this exemplary embodiment, the strips can have a width in therange of about 1 to about 5 inches. Other widths of the strips aresuitable. In this embodiment, the strips of material can be assembledinto two rings and wrapped around and attached to the wheel 140.Alternatively, the strips of material can be individually attached tothe wheel 140 in the desired configuration.

In an alternative exemplary embodiment (not illustrated in FIGS. 1A, 1B,2, and 14), the individual strips of material can be tapered on one orboth edges. Tapering the strips of material at the point of attachmentto the wheel 140 can allow for more complete overlap of the strips.Tapering the strips of material also can allow the strips to be attachedto two different wheel diameters, which can allow matching the strips tothe different diameters of different wheels 140. Additionally, taperingthe edges of the strips can allow forming the shape of the cavity toother suitable shapes. In an exemplary embodiment, the shape of thecavity can comprise a truncated cone.

A length of the layers 110, 120 equals the circumference of the wheel140 along the location 150. In an alternative exemplary embodiment, thelength of the layers 110, 120 can be greater than the circumference ofthe wheel 140 for overlapping ends of the layers 110, 120 when couplingthe layers 110, 120 to the wheel 140.

As shown in FIG. 1A, the layers 110, 120, are collapsed (or slack) closeto the wheel 140 when the wheel 140 is stationary. Tire rotationinflates/erects the layers 110, 120 by pulling the layers 110, 120outward from the center of the wheel 140. When a car on which the wheel140 is mounted is put into motion and the wheel 140 begins to rotate,centrifugal force forces the layers 110, 120 outward and forces theinner layer 120 together with the outer layer 110 to create theflow-resistant barrier. The layers 110, 120 are forced together suchthat the apertures 130 in the inner layer 120 are sealed by the outerlayer 110 and such that the apertures 130 in the outer layer 110 aresealed by the inner layer 120. Accordingly, the system 100 forms two aircavities 170, 180 in an internal air chamber of a tire mounted on thewheel 140, the internal air chamber being defined by the tire 160 andthe wheel 140. The outer air cavity 180 is formed on a tire (outer) sideof the layers 110, 120, and the inner air cavity 170 is formed on awheel 140 (inner) side of the layers 110, 120.

In an alternative exemplary embodiment, if the tire noise reducingdevice does not cover the air inlet (not shown) in the wheel, then theapertures 130 in the layers 110, 120 in the system 100 can be omitted.In this case, two continuous layers can form a two layer torus.

Alternatively, a single, continuous layer of flow-resistant materialwithout apertures 130 (i.e., without slits) can form a flow-resistantstructure that creates the inner and outer air cavities 170, 180. Theinternal air chamber of a tire can fully inflate without the apertures130 because the weave of the material does not entirely prevent airflow. In other words, the porosity of the material can allow for bothtire inflation when the wheel is stationary, and sufficientflow-resistant properties for the barrier to erect under centrifugalforce when the wheel is in motion. A similar continuous structure thatis formed in a curved shape is described hereinafter with reference toFIG. 11.

The layers 110, 120 restrict air flow between the two cavities 170, 180in the tire's internal air chamber. The “pores” (openings between theweave of the material) restrict but do not prevent such air flow. Thus,sound shock waves transmitted from the outer cavity 180 to the innercavity 170 and vice versa must pass through the layers 110, 120. Byresisting the air flow, the layers 110, 120 absorb the energy of theshock waves as the shock waves pass therethrough, thereby reducingnoise, in particular, reducing low-frequency noise in the range of about15 Hz to about 800 Hz and throughout the range of about 15 Hz to about20 kHz.

In another exemplary embodiment, the layers 110, 120 can slide acrosseach other and create friction when displaced by shock waves. Thisresulting friction reduces the low-frequency energy of the shock wavesby turning the shock waves'energy into heat, thereby further reducinglow-frequency noise associated with the low-frequency energy. Forexample, the two layers 110, 120 are held in place by centrifugal force.When the layers 110, 120 are displaced due to the concussion of soundenergy, the geometry of the elements induces a movement between thelayers 110, 120. Such movement causes friction between the layers 110,120. Converting the sound shock wave into heat reduces the sound energy.If the layers 110, 120 have one side that is rougher than the otherside, then the two rough sides can be disposed adjacent to each other toincrease the friction between the layers 110, 120. The increasedfriction can increase the frictional diaphragm effect to moreefficiently convert the sound energy into heat.

Additionally, a single-layer, continuous flow-resistant barrier canreduce noise via friction based on the movement of fibers within theweave of the material. The concussion f the sound energy moves thefibers with respect to each other, thereby causing friction within thebarrier and converting sound energy into heat to reduce the soundenergy.

In an exemplary embodiment, the outer layer 110 can comprise 3 inch wideportions between the apertures 130, and the inner layer 120 can comprise4 inch wide portions between its apertures 130. The additional width onone of the layers can increase a seal between the layers 110, 120 toform the flow-resistant barrier when rotated.

In another alternative exemplary embodiment illustrated in FIG. 14, thelayers 110, 120 can be coupled to the tire 160 which is then mounted onthe wheel 140. FIG. 14 is a cross-sectional view of a tire noiseabsorbing system 1400 comprising a flow-resistant barrier coupled to thetire 160 mounted to the wheel 140 according to an exemplary embodiment.As shown, the flow-resistant barrier comprises two layers 1402, 1404coupled to the tire 160 at locations 1406, which is mounted on the wheel140. The layers 1402, 1404 can comprise materials similar to thematerials of the layers 110, 120 described previously with reference toFIGS. 1A, 1B, 2, and 14. Accordingly, those materials can have similarflow-resistant properties to create a flow-resistant barrier and africtional noise attenuator. Additionally, the layers 1402, 1404 cancomprise a structure similar to the layers 110, 120 described previouslywith reference to FIGS. 1A, 1B, 2, and 14. Thus, the layers 1402, 1404have apertures 130 formed therein. The outer layer 1402 is offset fromthe inner layer 1404 such that the openings 130 of the outer and innerlayers 1402, 1404 do not overlap.

The layers 1402, 1404 can be coupled to the tire 160 in any suitablemanner. For example, the layers 1402, 1404 can be adhered to or moldedinto the bead or sidewalls of the tire 160. For instance, thesealternative exemplary embodiments include the following: weaving theedges of the layers 1402, 1404 into the tire 160, molding the layers1402, 1404 into the tire 160, inserting the layers 1402, 1404 into agroove in the tire casing, adhering the layers 1402, 1404 into or ontothe tire 160, or any other suitable method for coupling the layers 1402,1404 to the tire 160.

FIG. 3A is a perspective view illustrating a tire noise absorbing system300 comprising a flow-resistant barrier disposed on the wheel 140according to another exemplary embodiment. FIG. 3B a cross-sectionalview of the exemplary system 300 illustrated in FIG. 3A. As shown inFIGS. 3A and 3B, the system 300 comprises two layers 302, 304 ofmaterial attached to the wheel 140 to create an air flow-resistantbarrier. The layers 302, 304 can comprise materials similar to thematerials of the layers 110, 120 described previously with reference toFIGS. 1A, 1B, 2, and 14 and can be similarly coupled to wheel 140 ortire 160. Accordingly, those materials can have similar flow-resistantproperties to create a flow-resistant barrier and a frictional noiseattenuator. Additionally, the layers 302, 304 can comprise a structuresimilar to the layers 110, 120 described previously with reference toFIGS. 1A, 1B, 2, and 14. Thus, the layers 302, 304 have apertures 130formed therein. The outer layer 302 is offset from the inner layer 304such that the openings of the outer and inner layers 302, 304 do notoverlap. As illustrated, the system 300 comprises a lower profile thanthe system 100 illustrated in FIGS. 1A and 1B. The main differencebetween the systems 100 and 300 is that layers 302, 304 create aflow-resistant barrier having a lower profile than the flow-resistantbarrier created by the layers 110, 120. The size of the layers 302, 304can be adjusted to create the desired profile. A lower profile can makeit easier to mount the tire 160 over the layers 302, 304 on the wheel140.

FIG. 4A is a perspective view illustrating a tire noise absorbing system400 comprising a flow-resistant barrier disposed on the wheel 140according to yet another exemplary embodiment. FIG. 4B is across-sectional view of the exemplary system 400 illustrated in FIG. 4A.As shown in FIGS. 4A and 4B, the system 400 comprises two layers 402,404 of material attached to the wheel 140 to create an airflow-resistant barrier. The layers 402, 404 can comprise materialssimilar to the materials of the layers 110, 120 described previouslywith reference to FIGS. 1A, 1B, 2, and 14 and can be similarly coupledto the wheel 140 or tire 160. Accordingly, those materials can havesimilar flow-resistant properties to create a flow-resistant barrier anda frictional noise attenuator. Additionally, the layers 402, 404 cancomprise a structure similar to the layers 110, 120 described previouslywith reference to FIGS. 1A, 1B, 2, and 14. Thus, the layers 402, 404have apertures 130 formed therein. The outer layer 402 is offset fromthe inner layer 404 such that the apertures 130 of the outer and innerlayers 402, 404 do not overlap. As illustrated, the layers 402, 404 ofthe system 400 illustrated are attached to the wheel 140 at a morecentral location then the devices 100 and 300 discussed previously. Inother words, the layers 402, 404 are not attached to the outer portionof the wheel 140. Rather, the layers 402, 404 are attached closer to thecenter cross-section of the wheel 140. The configuration illustrated inFIGS. 4A and 4B can make it easier to install the layers 402, 404 to thewheel 140 without covering an air inlet valve (not shown) in the wheel140.

FIG. 5 is a perspective view illustrating a tire noise absorbing system500 comprising multiple elements 502 that create a flow-resistantbarrier according to an exemplary embodiment. The illustrated system 500comprises multiple, individual elements 502 with ends of adjacentelements 502 overlapping. As shown, the ends of adjacent elements 502can alternately overlap. In other words, each element 502 can have oneend that is overlapped by an adjacent element 502 and another end thatoverlaps another adjacent element 502.

Each element 502 can comprise materials similar to the materials of thelayers 110, 120 described previously with reference to FIGS. 1A, 1B, 2,and 14 and can be similarly coupled to wheel 140 or tire 160.Accordingly, those materials can have similar flow-resistant propertiesto create a flow-resistant barrier and a frictional noise attenuator.

In an exemplary embodiment, the elements 502 can be coupled one at atime to the wheel 140. Alternatively, the elements 502 can be coupledtogether at the outside edges to create a strip of elements 502 that canbe wrapped around and coupled to the wheel. In addition, a portion ofeach element 502 that is overlapped by an adjacent element 502 canremain unsecured from the wheel 140 at its edges. That configuration canallow greater tolerances in the manufacturing process.

Centrifugal force will force the elements 502 outward to contact eachother at the overlapped portions to create the flow-resistant barrier.Additionally, the overlapping portions of the elements 502 can rubtogether when deflected by sound shock waves, thereby creating frictionto convert the sound energy into heat and to attenuate the sound.Accordingly, the illustrated system 500 can provide diaphragm frictionand flow resistance to reduce noise within the tire 160 mounted to thewheel 140.

As shown in FIG. 5, the overlapping portions of the elements 502 aresecured to each other with a fastener 506 at the midpoint of theiroverlap. The fastener 506 can maintain the alignment between adjacentelements 502 and can help maintain the integrity of the inner air cavity170 created by the elements 502. In exemplary embodiments, fastener 506can comprise thin plastic fastener, thread, glue, staples, a sonic spotweld, or any other suitable material that can adequately hold adjacentelements 502 in place with respect to each other. Alternatively, theelements 502 can be left unsecured or can be secured with more than onefastener 506 at various locations along the overlap. The fastener 506 issuitable for use with other embodiments described herein to maintain thealignment of the flow-resistant barrier.

The elements 502 of the illustrated system 500 also can be mounted withor without covering the air intake valve (not shown) in the wheel 140and can provide more room to reliably mount the tire 160 to the wheel140.

FIG. 6A is a perspective view illustrating a tire noise absorbing system600 comprising multiple elements 602, 604 that create a flow-resistantbarrier according to another exemplary embodiment. FIG. 6B is a sideview of the exemplary system 600 illustrated in FIG. 6A. As shown inFIGS. 6A and 6B, the system 600 comprises multiple, individual elements602 that each overlap the ends of two adjacent elements 604 by an amount606. In other words, each element 602 has one end that overlaps anadjacent element 604 and another end that overlaps another adjacentelement 604. Each element 602 represents an outer element with respectto the wheel 140. Each element 604 represents an inner element withrespect to the wheel 140.

Each element 602, 604 can comprise materials similar to the materials ofthe layers 110, 120 described previously with reference to FIGS. 1A, 1B,2, and 14 and can be similarly coupled to wheel 140 or tire 160.Accordingly, those materials can have similar flow-resistant propertiesto create a flow-resistant barrier and a frictional noise attenuator.

In an exemplary embodiment, the elements 602, 604 can be coupled one ata time to the wheel 140 at location 150. Alternatively, the elements602, 604 can be coupled together at their outside edges to create astrip of elements 602, 604 that can be wrapped around and coupled to thewheel 140. In addition, a portion of each element 604 that is overlappedby an adjacent element 602 can remain unsecured from the wheel 140 atits edges. That configuration can allow greater tolerances in themanufacturing process.

FIG. 7 is a perspective view illustrating a tire noise absorbing system700 comprising discontinuous elements 702 coupled to the wheel 140according to an exemplary embodiment. The system 700 reduces noise viacontact friction. Each element 702 comprises two strips of overlappedmaterial, which move in relation to each other when concussed by a shockwave. The centrifugal force provided by the rotating wheel keeps the twostrips in contact with each other and the displacement between thestrips causes friction. The affect of the friction is to turn the audioshock wave into heat, thereby reducing the noise associated with theshock wave. In alternative exemplary embodiments, additional strips ofmaterial can be provided for each element 702. Additional alternativeexemplary embodiments can comprise only one element 702 or any number ofmultiple elements 702 coupled to the wheel 140.

FIG. 8A is a perspective view of a tire noise absorbing system 800comprising multiple elements 802 that create a flow-resistant barrieraccording to an exemplary embodiment. FIG. 8B is a cross-sectional viewof the exemplary system 800 illustrated in FIG. 8A. As shown in FIGS. 8Aand 8B, the system 800 comprises multiple interlocking elements 802 thateach comprises components 802 a, 802 b.

Component 802 a is an outer layer (with respect to the wheel 140) offlow-resistant material attached to the wheel 140 at location 150.Component 802 b is an inner layer (with respect to the wheel 140) offlow-resistant material that is attached to the wheel 140 only at itsedges beneath component 802 a. Thus, a space between the surfaces ofcomponents 802 a and 802 b exists.

Component 802 b is longer than component 802 a such that it protrudesbeyond component 802 a a distance of D. The portion of component 802 bthat extends beyond component 802 a is slightly narrower such that itsedges do not need to couple directly to the wheel 140. As shown, theillustrated system 800 comprises multiple continuous elements 802 withprotruding ends of each component 802 b of one element 802 interlockedbetween surfaces of components 802 a and 802 b of an adjacent element802. Centrifugal force will push the components 802 a, 802 b outward tocontact each other to create the flow-resistant barrier. Additionally,the components 802 a, 802 b will rub together, thereby creating frictionto convert sound energy into heat. Accordingly, the illustrated system800 can provide the diaphragm friction and flow resistance to reducenoise within a tire 160 mounted to the wheel 140.

The system 800 can provide an essentially-sealed, flow-resistant barrierwhen the tire is rotating, and sufficient air flow for tire inflationwhen the device is slack. In an exemplary embodiment, the components 802a, 802 b of each element 802 can be coupled together with thread,adhesive, or any other suitable material. Multiple adjacent elements 802can be coupled together at their edges to create a strip of elements 802that can be wrapped around and coupled to the wheel 140. Alternatively,the elements 802 can be individually coupled to the wheel 140.

The elements 802, either in a strip or individually, can be coupled tothe wheel 140 or tire 160 in a variety of ways as otherwise describedherein. For example, they can be glued to the wheel, fitted into agroove, or glued to the tire. In addition, adjacent elements 802 can besecured together using fasteners 506 as previously described withreference to FIG. 5.

The elements 802 can comprise materials similar to the materials of thelayers 110, 120 described previously with reference to FIGS. 1A, 1B, 2,and 14 and can be similarly coupled to the wheel 140 or tire 160.Accordingly, those materials can have flow-resistant properties tocreate a flow-resistant barrier and a frictional noise attenuator.

FIG. 9A is a perspective view illustrating a tire noise absorbing system900 comprising two or more elements 902, 904 that create multipleflow-resistant barriers according to an exemplary embodiment. FIG. 9B isa cross-sectional view of the exemplary system 900 illustrated in FIG.9A. As shown in FIGS. 9A and 9B, the elements 902, 904 represent onemore of the embodiments illustrated or described herein in one or moreof FIGS. 1-8. In addition, elements 902, 904 can represent one or moreof the embodiments described hereinafter in one or more of FIGS. 10-12.

In an exemplary embodiment, elements 902, 904 comprise the samestructure. Alternatively, elements 902, 904 can comprise differentstructures. For example, element 902 can comprise two overlappingcontinuous layers of material with openings therein as illustrated inany of FIGS. 1-4. Element 904 can be the same as element 902.Alternatively, element 904 can comprise any of the structuresillustrated in FIGS. 5-8 or 10-12, such as alternating overlappingelements as illustrated in FIG. 5.

Regardless of the structure of elements 902, 904, each element cancomprise materials similar to the materials of the layers 110, 120described previously with reference to FIGS. 1A, 1B, 2, and 14 and canbe similarly coupled to the wheel 140 or tire 160. Accordingly, thosematerials can have flow-resistant properties to create a flow-resistantbarrier and a frictional noise attenuator for each element 902, 904.

The two elements 902, 904 are coupled to the wheel 140 or tire 160 suchthat they form three flow-resistant air cavities within the internaltire air chamber. The inner air cavity 170 is formed between the wheel140 and the inner element 902. The middle air cavity 975 is formedbetween elements 902 and 904. The outer air cavity 180 is formed betweenelement 904 and the tire. In alternative exemplary embodiments,additional elements can be used to create more air flow-resistantbarriers and air cavities within the internal tire air chamber. Thecreation of multiple flow-resistant barriers restricts air flow througheach barrier and therefore absorbs noise associated with sound shockwaves passing therethrough. In an exemplary embodiment, the middle aircavity 975 can have a volume that less than the volume of the inner aircavity 170. In another exemplary embodiment, the middle air cavity 975can have a volume that is about 60-75 percent less than the volume ofthe inner air cavity 170.

In an exemplary embodiment, the elements 902, 904 can be coupled to eachother and then to the wheel 140 or tire 160 at location 150.Alternatively, each element can be coupled to the wheel or tireindividually at the same or separate locations. A variety of couplingmeans can be used as discussed herein including adhesives, clamps,insertion into a groove, or other suitable method.

As shown in FIGS. 9A and 9B, the elements 902, 904 create three aircavities 170, 180, 975 within the internal tire air chamber. Additionalelements can be used to create additional air cavities, if desired.Additionally, the air cavities 170, 180, 975 can be formed by couplingelements 902, 904 to the tire 160.

FIG. 10 is a perspective view illustrating a tire noise absorbing system1000 comprising a tubular air flow-resistant barrier 1002 according toanother exemplary embodiment. Barrier 1002 comprises a tubular elementof flow-resistant material woven in a curved shape such that it fits inthe internal tire air chamber defined by the wheel 140 and tire 160. Thecentrifugal force provided by the rotating wheel causes the tubularbarrier to erect and to fill with air, creating a flow-resistant cavitythat will absorb shock waves flowing through the barrier 1002 to reducetire noise.

The tubular barrier 1002 can be coupled around the wheel in a variety ofsuitable ways. For example, the tubular barrier 1002 can be tapered andcoupled at its ends, thus sealing the air cavity in one location. It canalso be weaved together to create a continuous circular air cavity. Suchan embodiment can be weaved or coupled in any other suitable way eitherdirectly around the wheel or in advance and then fitted over the wheel.The element 1002 then can be coupled to the wheel or tire.Alternatively, it can be left unsecured, staying in position byencompassing the circumference of the wheel 140.

The element 1002 can comprise materials similar to the materials of thelayers 110, 120 described previously with reference to FIGS. 1A, 1B, 2,and 14 and can be similarly coupled to wheel 140 or tire 160.Accordingly, those materials can have flow-resistant properties tocreate a flow-resistant barrier.

FIG. 11 is a perspective view illustrating a tire noise absorbing system1100 comprising a continuous flow-resistant barrier 1102 according to anexemplary embodiment. Barrier 1102 comprises a crescent-shaped elementwoven in a curved shape such that it fits around the wheel 140.Alternatively, the curvature of barrier 1102 can be semi-circular or anyother suitable curvature. For example, barrier 1102 can be curved suchthat it makes up 180 to 270 degrees of a circle, with its ends separatedby distance 1104. Barrier 1102 can be coupled to the tire or wheel byany suitable means described herein. Centrifugal force provided byrotating wheel 140 causes the barrier 1102 to erect and to fill withair, creating a flow-resistant barrier that will absorb shock wavesflowing through the element 1002 to reduce tire noise.

Barrier 1102 can comprise materials similar to the materials of thelayers 110,. 120 described previously with reference to FIGS. 1A, 1B, 2,and 14, but without apertures 130, and can be similarly coupled to wheel140 or tire 160. Accordingly, those materials can have flow-resistantproperties to create a flow-resistant barrier. At the same time, thematerial can still provide enough air flow to allow for complete tireinflation.

FIG. 12 is a perspective view illustrating a tire noise absorbing system1200 comprising multiple tubular air flow-resistant barriers 1202according to an exemplary embodiment. Barriers 1202 are tubular elementsweaved in a curved shape and then coupled to the wheel 140 or tire 160,creating multiple flow-resistant air cavities each similar to thosepreviously discussed with reference to FIG. 10. Alternatively, multipleelements 1202 can be coupled together at their ends 1204 to form acircle that will fit in the internal tire air chamber defined by thewheel 140 and the tire 160. The centrifugal force provided by therotating wheel will cause the barriers 1202 to erect and to inflate withair, creating separate flow-resistant cavities around the wheel 140.

FIG. 13 is a perspective view illustrating a representative element 1300that can be used in any embodiment illustrated in FIGS. 1-12 and 14according to an exemplary embodiment. Thus, FIG. 13 illustrates anelement 1300 whose characteristics can be used in the elements of any ofthe previously described embodiments to create a flow-resistant barrier.Element 1300 comprises a dampener 1302 arranged in a pattern lengthwisealong element 1300. Dampener 1302 can reduce the natural resonancevibration of the material, thus causing element 1300 to remain stifferunder high torque situations to maintain proper shape and to preventbreakage. The dampening can increase the absorbing performance becausethe absorber will have reduced performance if it is just vibrating inresonance with an existing sound source. Dampener 1302 can comprise apliable material such as silicone rubber, a permeable oil, thread,epoxy, an additional cloth element, or other suitable material. Thepliable material can add local stiffening to the element 1300 to createdifferent resonant characteristics for a particular type of cloth,thereby targeting a desired spectrum of low-frequency energy. Forexample, Dampener 1302 can be added to a single location, or,alternatively, it can be arranged in a pattern along element 1300,either cross-wise, length-wise, or in another suitable formation.

The element 1300 also comprises an attachment 1304. Attachment 1304comprises a material attached to the edges of element 1300 to produce acomposite edge that provides ease and efficiency in attaching theelement 1300 to either the wheel 140 or tire 160. This coupling optionprovides a possible alternative to the previously mentioned couplingoptions. Attachment 1304 comprises a material that will couple moreeasily to the wheel 140 or tire 160 than the material of element 1300will couple to those items. In alternative exemplary embodiments,attachment 1304 can comprise plastic, cotton, fabric, metal, or anyother suitable material for coupling the element 1302 to the wheel 140or the tire 160.

Attachment 1304 can be attached to the material of element 1300 withadhesive, thread, or other suitable means. As illustrated in FIG. 13,attachment 1304 comprises a strip of suitable material coupled toelement 1300 along the length of the edges of element 1300.Alternatively, attachment 1304 can comprise smaller, distinct piecesthat are attached repeatedly along the edges of element 1300.

The element 1300 can comprise materials similar to the materials of thelayers 110, 120 described previously with reference to FIGS. 1A, 1B, 2,and 14 and can be similarly coupled to wheel 140 or tire 160.Accordingly, those materials can have flow-resistant properties tocreate a flow-resistant barrier and a frictional noise attenuator.

As discussed herein, a tire noise reducing device can comprisecontinuous air flow-resistant layers of overlapped material withopenings therein; a single flow-resistant and continuous layer withoutopenings; multiple individual elements with overlapping and/orinterlocking end portions; multiple discontinuous elements; two or morelayers of elements that create multiple flow-resistant barriers; asingle tubular element; a semicircular element; or multiple tubularelements.

In exemplary embodiments, small production runs for the material of theflow-resistant barriers described herein can comprise laser cutting thelayers or individual elements to the specific wheel and tire dimensions.Large production runs can be die cut.

According to an exemplary embodiment, the tire noise absorbing systemsdescribed herein can absorb sound in the full audio band of about 15 Hzto about 20 kHz. Since some tire structures do not include noise infrequencies significantly above 800 Hz, the tire noise absorbing systemsdescribed herein also can absorb sound in a range of about 15 Hz toabout 800 Hz. Additionally, varying the material of the flow-resistantbarrier and the size of the cavity defined by the barrier can adjust thesound frequency absorbing characteristics of the systems to a desiredrange.

The tire noise absorbing systems according to the exemplary embodimentsdescribed herein can provide several benefits. For example, reducinginternal tire energy can reduce tire structure hysteresis. This affectcan increase tread adhesion by reducing the energy that causes treadcontact bounce. Further, reducing hysteresis can reduce the tiretemperature, which can allow a tire manufacturer to use tire compoundswith greater adhesion but lower maximum temperature. Reducing tiretemperature also can extend the life of tires under racing conditions.For commercial applications, the reduction of temperature and theincrease of adhesion can result in lower rolling resistance and greatertire life. This affect would result in significantly lower operatingcosts for applications such as heavy trucks and public transit. Each ofthese improvements can result in tire and automobile performanceimprovements.

The device increases tire life by absorbing energy inside the tire,thereby reducing contact bounce. This reduction increases adhesion ofthe tire to the road surface, which can reduce the scrubbing movementbetween the tire and road surface. Since scrubbing off rubber byadhesion slip is a large cause of tire wear, the tire noise absorbingsystems can increase the dynamic performance and adhesion of a tire.

In an alternative exemplary embodiment (not shown), one or moremicro-perforated metal layers can be used instead of cloth layers. Themetal layers can be formed to have the desired shape around thecircumference of the wheel 140, can be coupled to the wheel 140 or to atire 160 mounted on the wheel 140, and can create an inner and outer aircavity 170, 180 between the tire 160 and the wheel 140. The perforationsin the layers can restrict air flow between the outer and inner cavities170, 180, thereby absorbing low-frequency energy of shock wavestransmitted between the outer and inner cavities 170, 180 and viceversa. Additionally, if multiple layers are used, the shock waves cancause the multiple layers to move relative to each other, therebyabsorbing additional energy by converting friction energy into heat.According to an exemplary embodiment, the perforations on the metallayers can produce a porosity in the range of about 10% to about 50%cavity fill at cavity saturation.

Although specific embodiments have been described above in detail, thedescription is merely for purposes of illustration. Variousmodifications of, and equivalent steps corresponding to, the disclosedaspects of the exemplary embodiments, in addition to those describedabove, can be made by those skilled in the art without departing fromthe spirit and scope of the invention defined in the following claims,the scope of which is to be accorded the broadest interpretation so asto encompass such modifications and equivalent structures.

1. A system for dissipating sound shock waves, comprising: a wheel upon which a tire can be mounted to create an internal air chamber defined by said wheel and the tire; a flow-resistant barrier coupled to said wheel and defining an air cavity within the internal air chamber, said barrier comprising a material that provides an acoustical resistance to sound shock waves passing therethrough, the air cavity defined by said barrier having a volume such that air within the cavity offers relatively small impedance to the passage of shock waves through said barrier and into the air cavity.
 2. The system according to claim 1, wherein centrifugal force erects said barrier around said wheel to create the air cavity.
 3. The system according to claim 1, wherein said barrier produces frictional heat when displaced by a shock wave, thereby converting energy of the shock wave to heat to reduce noise associated therewith.
 4. The system according to claim 1, wherein said barrier is coupled to said wheel using at least one method selected from the group consisting of gluing, crimping, molding, and welding.
 5. The system according to claim 1, wherein said barrier comprises a dampening element that changes a resonant frequency of the system.
 6. The system according to claim 1, wherein said barrier comprises a continuous layer of flow-resistant material disposed around said wheel.
 7. The system according to claim 1, wherein said barrier comprises a plurality of layers disposed adjacent to each other, wherein each of said layers comprises a plurality of apertures, and wherein adjacent ones of said layers are disposed such that the apertures in adjacent layers are offset.
 8. The system according to claim 7, wherein each of said layers comprises a layer edge corresponding to the circumference of said wheel, and wherein said layers are coupled together at their respective layer edges.
 9. The system according to claim 7, wherein said barrier comprises a barrier edge corresponding to the circumference of said wheel, and wherein said barrier is coupled around said wheel at the barrier edge.
 10. The system according to claim 1, wherein said barrier comprises a plurality of overlapping elements disposed continuously around said wheel such that each of said elements overlaps an end of an adjacent one of said elements.
 11. The system according to claim 1, wherein said barrier comprises a plurality of elements disposed continuously around said wheel such that every other one of said elements is overlapped on one of its ends by an adjacent one of said elements and is overlapped on another one of its ends by another adjacent one of said elements.
 12. The system according to claim 1, wherein said barrier comprises a plurality of interlocking elements disposed continuously around said wheel.
 13. The system according to claim 1, wherein each of said elements comprises two components of flow-resistant material with a first component being longer than a second component, wherein said interlocking elements are disposed continuously around said wheel such that the longer component of each one of said elements is disposed between the longer and short components of an adjacent one of said elements.
 14. The system according to claim 1, wherein said flow-resistant barrier defines a plurality of air cavities within the internal air chamber, wherein said barrier providing an acoustical resistance to sound shock waves passing therethrough into each of the air cavities, and wherein each of the air cavities has a volume such that air within a respective air cavity offers relatively small impedance to the passage of shock waves through said barrier and into the respective air cavity.
 15. The system according to claim 1, wherein said flow-resistant barrier comprises at least one tubular-shaped flow-resistant barrier disposed around said wheel.
 16. The system according to claim 1, wherein said flow-resistant barrier comprises a plurality of tubular-shaped flow-resistant barriers disposed around said wheel.
 17. The system according to claim 1, further comprising the tire mounted to said wheel.
 18. A system for dissipating sound shock waves, comprising: a tire that can be mounted to a wheel to create an internal air chamber defined by said tire and the wheel; a flow-resistant barrier coupled to said tire and defining an air cavity within the internal air chamber, said barrier comprising a material that provides an acoustical resistance to sound shock waves passing therethrough, the air cavity defined by said barrier having a volume such that air within the cavity offers relatively small impedance to the passage of shock waves through said barrier and into the air cavity.
 19. The system according to claim 18, further comprising the wheel, wherein said tire is mounted to said wheel.
 20. A device for dissipating sound shock waves, comprising: a flow-resistant barrier that defines an air cavity within an internal air chamber created by a tire mounted to a wheel, said barrier comprising a material that provides an acoustical resistance to sound shock waves passing therethrough, the air cavity defined by said barrier having a volume such that air within the cavity offers relatively small impedance to the passage of shock waves through said barrier and into the air cavity.
 21. The system according to claim 20, further comprising the wheel, wherein said barrier is attached to said wheel.
 22. The system according to claim 20, further comprising the tire, wherein said barrier is attached to said tire.
 23. The system according to claim 20, further comprising the wheel and the tire, wherein said barrier is attached to one of said wheel and said tire.
 24. A system for dissipating noise-producing shock waves, comprising: a least one element disposed in an internal air chamber defined by a wheel and a tire, said element comprising at least two components, wherein said components produce frictional heat when displaced by a shock wave, thereby converting energy of the shock wave to heat to reduce noise associated therewith.
 25. The system according to claim 24, wherein centrifugal force causes said components for each of said elements to contact each other.
 26. The system according to claim 24, further comprising the wheel, wherein said elements are coupled to said wheel.
 27. The system according to claim 24, further comprising the tire, wherein of said elements are coupled to said tire. 